2021
DOI: 10.1101/2021.09.27.461996
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Rapid parameter estimation for selective inversion recovery myelin imaging using an open-source Julia toolkit

Abstract: Background: Magnetic resonance imaging (MRI) is used extensively to quantify myelin content, however computational bottlenecks remain challenging for advanced imaging techniques in clinical settings. We present a fast, open-source toolkit for processing quantitative magnetization transfer derived from selective inversion recovery (SIR) acquisitions that allows parameter map estimation, including the myelin-sensitive macromolecular pool size ratio (PSR). Significant progress has been made in reducing SIR acquis… Show more

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“…Substituting Equation ( 12) into Equation ( 13) and using Equations ( 5)-( 9), the resultant longitudinal magnetization of the free pool M f (t i ) contains seven parameters: R 1f , R 1m , PSR, k mf , S f , S m , and M f (∞), which can be estimated by fitting the measured data to the above bi-exponential model. 21,22,40 During fitting, k mf can be assumed a constant value (= 12.5 s −1 ) as it was shown to be relatively consistent in normal and diseased neural tissue. 41 Furthermore, it has been shown errors in the assumed k mf value do not significantly bias estimates of the other model parameters when the optimal sampling strategies are used.…”
Section: Theorymentioning
confidence: 99%
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“…Substituting Equation ( 12) into Equation ( 13) and using Equations ( 5)-( 9), the resultant longitudinal magnetization of the free pool M f (t i ) contains seven parameters: R 1f , R 1m , PSR, k mf , S f , S m , and M f (∞), which can be estimated by fitting the measured data to the above bi-exponential model. 21,22,40 During fitting, k mf can be assumed a constant value (= 12.5 s −1 ) as it was shown to be relatively consistent in normal and diseased neural tissue. 41 Furthermore, it has been shown errors in the assumed k mf value do not significantly bias estimates of the other model parameters when the optimal sampling strategies are used.…”
Section: Theorymentioning
confidence: 99%
“…And finally, at the end of the inversion time, the longitudinal magnetization of the free pool (that is proportional to the acquired signal intensity) is Mf()tigoodbreak=()bf+()tieR1+tigoodbreak+bf()tieR1tigoodbreak+1Mf().$$ {M}_f\left({t}_i\right)=\left({b}_f^{+}\left({t}_i\right){e}^{-{R}_1^{+}{t}_i}+{b}_f^{-}\left({t}_i\right){e}^{-{R}_1^{-}{t}_i}+1\right)\cdot {M}_f\left(\infty \right). $$ Substituting Equation () into Equation () and using Equations (), the resultant longitudinal magnetization of the free pool Mf()ti$$ {M}_f\left({t}_i\right) $$ contains seven parameters: R1f$$ {R}_{1f} $$, R1m$$ {R}_{1m} $$, italicPSR$$ PSR $$, kmf$$ {k}_{mf} $$, Sf$$ {S}_f $$, Sm$$ {S}_m $$, and Mf()$$ {M}_f\left(\infty \right) $$, which can be estimated by fitting the measured data to the above bi‐exponential model 21,22,40 …”
Section: Theorymentioning
confidence: 99%